Page 414 - 35Linear Algebra
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                            we have
                                                                   
                                                                   2
                                                           Lv =   −2   = 2v
                                                                   4

                            so v ∈ E (2) . In general, we note the linearly independent vectors v (λ)  with the
                                                                                              i
                                                                                   P   i (λ)
                            same eigenvalue λ span an eigenspace since for any v =    c v  , we have
                                                                                     i   i
                                                  X   i  (λ)  X   i  (λ)   X   i (λ)
                                             Lv =    c Lv   =    c λv   = λ   c v   = λv.
                                                         i           i           i
                                                   i           i            i

                            Hint for Review Problem 9

                            We are looking at the matrix M, and a sequence of vectors starting with

                                   x(0)
                            v(0) =       and defined recursively so that
                                    y(0)

                                                              x(1)       x(0)
                                                      v(1) =       = M         .
                                                              y(1)       y(0)
                            We first examine the eigenvectors and eigenvalues of


                                                                   3  2
                                                            M =         .
                                                                   2  3
                            We can find the eigenvalues and vectors by solving

                                                           det(M − λI) = 0

                            for λ.

                                                             3 − λ   2
                                                        det               = 0
                                                               2   3 − λ
                            By computing the determinant and solving for λ we can find the eigenvalues λ =
                            1 and 5, and the corresponding eigenvectors. You should do the computations
                            to find these for yourself.
                               When we think about the question in part (b) which asks to find a vector
                            v(0) such that v(0) = v(1) = v(2) . . ., we must look for a vector that satisfies
                            v = Mv. What eigenvalue does this correspond to? If you found a v(0) with
                            this property would cv(0) for a scalar c also work? Remember that eigenvectors
                            have to be nonzero, so what if c = 0?
                               For part (c) if we tried an eigenvector would we have restrictions on what
                            the eigenvalue should be? Think about what it means to be pointed in the same
                            direction.


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